| 研究生: |
朱冠霖 Chu, Kuan-Lin |
|---|---|
| 論文名稱: |
液態噴流注入超音速流場之數值模擬分析 Numerical Simulation of Liquid Jet Injection into a Supersonic Flow |
| 指導教授: |
江滄柳
Jiang, Tsung-Leo |
| 學位類別: |
碩士 Master |
| 系所名稱: |
工學院 - 航空太空工程學系 Department of Aeronautics & Astronautics |
| 論文出版年: | 2015 |
| 畢業學年度: | 103 |
| 語文別: | 中文 |
| 論文頁數: | 86 |
| 中文關鍵詞: | 超音速流場 、K-H/R-T 破碎模型 、數值模擬 |
| 外文關鍵詞: | Supersonic flow, K-H/R-T breakup model, Numerical simulation |
| 相關次數: | 點閱:107 下載:4 |
| 分享至: |
| 查詢本校圖書館目錄 查詢臺灣博碩士論文知識加值系統 勘誤回報 |
在超音速流場內之液態噴流具有複雜之物理現象,因為,其牽涉到噴霧在超音速紊流場中之霧化與蒸發,以及震波與邊界層之交互作用等複雜之物理問題。因此,對霧化機制之了解有助於分析探討液態燃料在超音速燃燒衝壓引擎之霧化及燃燒現象。目前液態燃料的使用,為不可避免之趨勢,但液態燃料需考慮燃料霧化程度、蒸發過程以及燃燒延遲等現象,因此增添流場之複雜性。然而實驗在觀察如此之迅速的物理現象上較為困難,為此需建立一合理之噴霧數值模型,模擬複雜流場之物理現象,因此本文將使用CFD 計算流體力學,ANSYS FLUENT 軟體,進行液態水注入超音速流場之數值模擬計算,紊流模式採用SST K-ω,霧化模式則採用Kelvin-Helmholtz/Rayleigh-Taylor(K-H/R-T)破碎模式。本研究針對KH/R-T破碎參數做分析,探討不同參數對超音速流場之噴霧結構的影響,發現CL參數對K-H model 和R-T model 之作用區域以及作用程度有非常大的關係,且粒徑參數比時間參數更能主導穿透高度之趨勢。再者,針對液態碳氫燃料注入超音速流場之模擬分析,首先進行不同噴注速度之分析,發現在比較噴注速度為78m/s 及85m/s 時,噴注速度越大弓形震波產生之壓力越大,且角度也越大,越容易注入流場內。接著進行不同噴注角度之分析,發現在比較噴注角度30 度、45 度及垂直上噴時,噴注45 度液滴的碎裂霧化效果最好。之後進行不同燃料溫度之分析,發現在比較攝氏30 度、攝氏100 度及攝氏130 度之燃料溫度後,攝氏130 度之煤油蒸發效果最好,蒸發量也最多。
In the present study, the CFD software ANSYS-FLUENT was employed to conduct a numerical simulation of water and liquid-hydrocarbon fuel injection in a supersonic flow,
respectively. Both the SST k-ω turbulence model and the K-H/R-T breakup model were adopted for this analysis. Through analyzing the different parameters of the K-H/R-T model affecting the water-jet breakup and atomization, it was found that the effective area of K-H model extended as the CL parameter, which controls the length of liquid core region, increased. The penetration height was much more dominated by particle size parameters such as B0 and CRT than it was by time parameters like B1 and Ctau. When comparing the injection speed at 75m/s with that at 80m/s for liquid-hydrocarbon fuel injection in a supersonic flow, it could be seen that a faster speed may increase the pressure behind the bow shock and angle of the bow shock wave. Furthermore, atomization at a forward angle of 45-degree relative to vertical direction turns out to be the most effective method by which to compare a forward angle of 30-degree and a vertical injection. When analyzing the evaporation effects of the fuel temperature at 30℃, 100℃and 130℃ separately, it was found that evaporation worked best at a temperature of 130℃.
[1] Ali, M., Fujiwara, T., and Leblanc, J. E., "Influence of main
flow inlet configuration on mixing and flameholding in transverse
injection into supersonic airstream," International Journal of Engineering
Science, Vol. 38, No. 11, pp. 1161-1180, 2000.
[2] Ali, M., Sadrul Islam, A. K. M., and Ahmed, S., "Mixing and
flame holding with air inlet configuration in scramjet combustor,"
International communications in heat and mass transfer, Vol. 31, No. 8,
pp. 1187-1198, 2004.
[3] Ali, M. and Sadrul Islam, A. K. M., "Study on main flow and
fuel injector configurations for scramjet applications," International
Journal of Heat and Mass Transfer, Vol. 49, No. 19, pp. 3634-3644, 2006.
[4] Ben-Yakar, A. and Hanson, R. K., "Experimental
investigation of flame-holding capability of hydrogen transverse jet in
supersonic cross-flow," Twenty-Seventh International Symposium on
Combustion, Combustion Institute, Vol. 27, pp. 2173-2180, 1998.
[5] Powell, O. A., Edwards, J. T., Norris, R. B., Numbers, K. E.,
and Pearce, J. A., "Development of hydrocarbon-fueled scramjet engines:
the hypersonic technology (HyTech) Program," Journal of Propulsion
and Power, Vol. 17, No. 6, pp. 1170-1176, 2001.
[6] Lewis, M. J., "Significance of fuel selection for hypersonic
vehicle range," Journal of Propulsion and Power, Vol. 17, No. 6, pp.
1214-1221, 2001.
[7] Waltrup, P. J., "Upper bounds on the flight speed of
hydrocarbon-fueled scramjet-powered vehicles," Journal of Propulsion
and Power, Vol. 17, No. 6, pp. 1199-1204, 2001.
[8] Tetlow, M. R. and Doolan, C. J., "Comparison of hydrogen
and hydrocarbon-fueled scramjet engines for orbital insertion," Journal
of Spacecraft and Rockets, Vol. 44, No. 2, pp. 365-373, 2007.
[9] Amati, V., Bruno, C., Simone, D., and Sciubba, E., "Exergy
analysis of hypersonic propulsion systems: Performance comparison of
two different scramjet configurations at cruise conditions," Energy, Vol.
33, No. 2, pp. 116-129, 2008.
[10] Kush, E. A. and Schetz, J. A., "Liquid jet injection into a
supersonic flow," AIAA Journal, Vol. 11, No. 9, pp. 1223-1224, 1973.
84
[11] Lander, H. and Nixon, A. C., "Endothermic fuels for
hypersonic vehicles," Journal of Aircraft, Vol. 8, No. 4, pp. 200-207,
1971.
[12] Menter, F. R., "Two-equation eddy-viscosity turbulence
models for engineering applications," AIAA Journal, Vol. 32, No. 8, pp.
1598-1605, 1994.
[13] Chenault, C. F., Beran, P. S., and Bowersox, R. D. W.,
"Numerical investigation of supersonic injection using a Reynolds-stress
turbulence model," AIAA Journal, Vol. 37, No. 10, pp. 1257-1269, 1999.
[14] Liu, O. Z., Cai, Y. H., Hu, Y. L., Liu, J. H., and Ling, W. H.,
"The turbulence models for numerical analysis of liquid kerosene
supersonic combustion," Acta Aerodynamica Sinica, Vol. 25, No. 3, pp.
362-367, 2007.
[15] 宋緯倫, "不同紊流模式對超音速流場數值模擬結果之影
響," 成功大學航空太空工程學系碩士論文, pp. 1-70, 2010.
[16] Aso, S., Okuyama, S., Kawai, M., and Ando, Y.,
"Experimental study on mixing phenomena in supersonic flows with slot
injection," AIAA paper, Vol. 16, 1991.
[17] Arai, T. and Schetz, J. A., "Injection of bubbling liquid jets
from multiple injectors into a supersonic stream," Journal of Propulsion
and Power, Vol. 10, No. 3, pp. 382-386, 1994.
[18] Lin, K. C., Kirkendall, K. A., Kennedy, P. J., and Jackson, T.
A., "Spray structure of aerated liquid fuel jets in supersonic crossflows,"
AIAA paper, pp. 1999-2374, 1999.
[19] Yu, G., Li, J. G., Yang, S. R., Yue, L. J., Zhang, X. Y., Huang,
Y., and Sung, C. J., "Investigation of liquid hydrocarbon combustion in
supersonic flow using effervescent atomization," AIAA paper, pp. 2002-
4279, 2002.
[20] Yue, L. J. and Yu, G., "Studies on spray characteristics of
barbotaged atomizer," Journal of Propulsion Technology, Vol. 24, No. 4,
2003.
[21] Yu, G., Li, J. G., Zhao, J. R., Yue, L. J., Chang, X. Y., and
Sung, C. J., "An experimental study of kerosene combustion in a
supersonic model combustor using effervescent atomization,"
Proceedings of the Combustion Institute, Vol. 30, No. 2, pp. 2859-2866,
85
2005.
[22] Qian, L. j., Lin, J. Z., and Xiong, H. B., "Simulation of
droplet-gas flow in the effervescent atomization spray with an impinging
plate," Chinese Journal of Chemical Engineering, Vol. 17, No. 1, pp. 8-
19, 2009.
[23] Wang, L., Zhang, C. L., Wei, B. X., and Xu, X., "Experimental
investigation of kerosene supersonic combustion test using aerated liquid
injectors," Journal of Aerospace Power, Vol. 24, No. 2, 2009.
[24] Less, D. M. and Schetz, J. A., "Transient behavior of liquid
jets injected normal to a high-velocity gas stream," AIAA Journal, Vol.
24, No. 12, pp. 1979-1986, 1986.
[25] Heister, S. D., Nguyen, T. T., and Karagozian, A. R.,
"Modeling of liquid jets injected transversely into a supersonic
crossflow," AIAA Journal, Vol. 27, No. 12, pp. 1727-1734, 1988.
[26] Wu, P. K., Kirkendall, K. A., Fuller, R. P., and Nejad, A. S.,
"Breakup processes of liquid jets in subsonic crossflows," Journal of
Propulsion and Power, Vol. 13, No. 1, pp. 64-73, 1997.
[27] Yue, L. J. and Yu, G., "Numerical simulation of kerosene
spray in supersonic cross flow," Journal of Propulsion Technology, Vol.
25, No. 1, pp. 11-14, 2004.
[28] Im, K. S., Lin, K. C., and Lai, M. C., "Spray atomization of
liquid jet in supersonic cross flows," AIAA paper, Vol. 732, 2005.
[29] Im, K.-S., Lin, K.-C., Lai, M.-C., and Chon, M. S., "Breakup
modeling of a liquid jet in cross flow," International Journal of
Automotive Technology, Vol. 12, No. 4, pp. 489-496, 2011.
[30] Yang, S. H. and Le, J. L., "Numerical simulation of liquid fuel
atomization in supersonic crossflow," Journal of Propulsion Technology,
Vol. 29, No. 5, pp. 519-522, 2008.
[31] Wang, J. F., Liu, C., and Wu, Y. H., "Numerical simulation of
spray atomization in supersonic flows," Modern Physics Letters B, Vol.
24, No. 13, pp. 1299-1302, 2010.
[32] Liu, J. and Xu, X., "Numerical simulation of atomization of
liquid jet in supersonic crossflow," Journal of Beijing University of
Aeronautics and Astronautics, Vol. 36, No. 10, pp. 1166-1170, 2010.
[33] Liu, H. X., Guo, Y. C., and Lin, W. Y., "Numerical
investigation of liquid jet injection into a supersonic crossflow," 29th
Congress of the International Council of the Aeronautical Sciences, 2014.
86
[34] Yang, D. C., Zhu, W. B., Chen, H., Guo, J. X., and Liu, J. W.,
"Modeling the secondary breakup of a liquid jet in supersonic cross
flows," Journal of Harbin Engineering University, Vol. 35, No. 1, pp. 62-
68, 2014.
[35] Lin, K. C., Kennedy, P. J., and Jackson, T. A., "Structures of
water jets in a Mach 1.94 supersonic crossflow," AIAA paper, Vol. 971,
2004.
[36] Ranz, W. E. and Marshall, W. R., "Evaporation from drops,"
Chemical Engineering Progress (CEP) magazine, Vol. 48, No. 3, pp. 141-
146, 1952.
[37] FLUENT, "15.0 User's Guide," ANSYS Inc, 2013.
[38] Beale, J. C. and Reitz, R. D., "Modeling spray atomization
with the Kelvin-Helmholtz/Rayleigh-Taylor hybrid model," Atomization
and sprays, Vol. 9, No. 6, 1999.
[39] 沈雅蓁, "側向雙垂直噴注於超音速空氣流場之霧化混合
探討," 成功大學航空太空工程學系碩士論文, 2015.
[40] 黃泓賓, "熱焓變化對超音速流場中側向噴流霧化的現向
觀察," 成功大學航空太空工程學系碩士論文, 2015.